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SLOPE FAILURE ASSESSMENT IN PENANG ISLAND USING GEOELECTRICAL METHODS by MUHAMAD IQBAL MUBARAK FAHARUL AZMAN Thesis submitted in fulfilment of the requirements for the degree of Master in Science April 2018

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  • SLOPE FAILURE ASSESSMENT

    IN PENANG ISLAND

    USING GEOELECTRICAL METHODS

    by

    MUHAMAD IQBAL MUBARAK

    FAHARUL AZMAN

    Thesis submitted in fulfilment of the requirements

    for the degree of

    Master in Science

    April 2018

  • ii

    ACKNOWLEDGEMENT

    I thank Allah S.W.T for His mercy for giving me this opportunity to further

    study in Master’s degree and His guidance for me to face challenges in order to

    complete this research.

    I would like to express my sincere gratitude to my main supervisor, Dr Nur

    Azwin Ismail for her continuous support, guidance and encouragement that leads me

    to completing my research. A special thanks to my co – supervisor, Dr Nordiana Mohd

    Muztaza for her invaluable advices and suggestions. Many thanks also to all

    Geophysics laboratory assistants for their time and effort in assisting me to conduct

    my research.

    My appreciation also to all my very helpful and supportive postgraduate

    students for their non – stop encouragement and knowledge sharing that allow me to

    move forward.

    My sincere appreciation toward my beloved parents Mr. Faharul Azman

    Ahmad Sabki and Mrs. Faridah Md Saad and also my siblings for their prayers and

    encouragements. Last but not least, Fellowship Scheme of Universiti Sains Malaysia

    for sponsoring my tuition fees and allowances during my study period.

  • iii

    TABLE OF CONTENTS

    Acknowledgement ii

    Table of Contents iii

    List of Tables vii

    List of Figures x

    List of Abbreviations xiv

    List of Symbols xvi

    Abstrak xviii

    Abstract xx

    CHAPTER 1: INTRODUCTION

    1.0 Preface 1

    1.1 Problem statements 3

    1.2 Research objectives 5

    1.3 Scope of research 5

    1.4 Significant of study 6

    1.5 Thesis outlines 7

    CHAPTER 2: LITERATURE REVIEW

    2.0 Introduction 8

    2.1 Previous studies 8

    2.2 Basic theory of 2D resistivity method 25

    2.3 Basic theory of induced polarization 28

    2.4 Depth of penetration 30

  • iv

    2.5 Porosity 30

    2.6 Moisture content 31

    2.7 Bulk density 31

    2.8 Summary 32

    CHAPTER 3: MATERIALS AND METHODS

    3.0 Introduction 33

    3.1 Geology and geomorphology of Penang Island 34

    3.2 Study area 37

    3.2.1 Sungai Batu 42

    3.2.2 Bukit Relau 43

    3.2.3 Air Hitam 44

    3.3 Laboratory test 45

    3.3.1 Moisture content measurement 46

    3.3.2 Porosity calculation 46

    3.3.3 Particle size distribution (PSD) analysis 47

    3.3.3(a) Experiment procedure 48

    3.3.3(b) Coefficient of gradation, Cc and coefficient

    of uniformity, Cu

    48

    3.3.3(c) Particle size statistics of mean and sorting 50

    3.4 Geophysical methods 51

    3.4.1 2D resistivity method 52

    3.4.2 Induced polarization (IP) method 54

    3.4.3 Electrical properties of materials 54

    3.4.4 Data acquisition 55

  • v

    3.4.5 Data processing 57

    3.5 Monitoring the study area 58

    3.6 Rainfall distribution 59

    3.7 Regression analysis 60

    3.8 Summary 61

    CHAPTER 4: RESULTS AND DISCUSSION

    4.0 Introduction 63

    4.1 Results 63

    4.1.1 Sungai Batu 64

    4.1.1(a) Laboratory test 64

    4.1.1(b) Particle size distribution (PSD) analysis

    65

    4.1.1(c) Rainfall distribution 67

    4.1.1(d) Geophysical methods 69

    4.1.1(e) Slope monitoring 71

    4.1.1(f) Changes within Sungai Batu study area

    subsurface

    75

    4.1.2 Bukit Relau 81

    4.1.2(a) Laboratory test 81

    4.1.2(b) Particle size distribution (PSD) analysis

    82

    4.1.2(c) Rainfall distribution 84

    4.1.2(d) Geophysical methods 86

    4.1.2(e) Slope monitoring 88

    4.1.2(f) Changes within Bukit Relau study area

    subsurface

    91

    4.1.3 Air Hitam 93

  • vi

    4.1.3(a) Laboratory test 93

    4.1.3(b) Geophysical methods 94

    4.2 Empirical correlation between soil moisture content and porosity

    96

    4.3 Empirical correlation between geophysical data and laboratory

    tests

    97

    4.4 Empirical correlation between geophysical data and rainfall

    distribution

    99

    4.5 Summary 101

    CHAPTER 5: CONCLUSION AND RECOMMENDATIONS

    5.0 Conclusion 105

    5.1 Recommendations for future work 109

    REFERENCES 110

    APPENDICES

  • vii

    LIST OF TABLES

    Page

    Table 1.1 Series of major slope failure occurrences in Malaysia and

    consequences in terms of deaths from 2002 – 2017.

    1

    Table 1.2 Summary of slope failures in Penang Island.

    4

    Table 2.1 Summary of resistivity value with interpretation at the study

    areas in Selangor (Muztaza et al., 2017).

    17

    Table 2.2 Resistivity range of weathered granite and fresh granite in

    Malaysia (Yaccup and Tawnie, 2015).

    18

    Table 2.3 Saturated peak shear box and particle size distribution tests

    (Hashim et al., 2015).

    24

    Table 2.4 Result of soil classification and particle size distribution test

    (Hashim et al., 2015).

    24

    Table 2.5 Porosity of soil according to the percentage of porosity (Faur

    and Szabo, 2011).

    31

    Table 2.6 Relationship of soil bulk density for root growth based on

    soil texture (Arshad et al., 1996).

    31

    Table 3.1 Description of weathering grade (Attewell, 1993).

    41

    Table 3.2 Name of equipment as labelled in Figure 3.11.

    45

    Table 3.3 Name of equipment as labelled in Figure 3.12.

    48

    Table 3.4 Summary of soil classification (Santamarina et al., 2001).

    49

    Table 3.5 Conversion from millimetre to phi unit (Folk and Ward,

    1957).

    50

    Table 3.6 Values of sorting and the interpretation (Folk and Ward,

    1957).

    51

    Table 3.7 Resistivity of various rock and sediment (Telford, 1990).

    55

    Table 3.8 Chargeability of various material (Telford, 1990).

    52

    Table 3.9 Name of equipment as labelled in Figure 3.16.

    57

    Table 3.10 Categories of precipitation and the description (Department

    of Meteorological Malaysia, 2018).

    59

  • viii

    Table 3.11 Strength of correlation (Evan, 1996).

    60

    Table 4.1 Laboratory test for Sungai Batu study area.

    64

    Table 4.2 Particle size distribution analysis result at Sungai Batu study

    area.

    65

    Table 4.3 Mean and standard deviation of Sungai Batu soil samples.

    66

    Table 4.4 Summary of resistivity value with interpretation and feature

    found at Sungai Batu study area.

    69

    Table 4.5

    Summary of chargeability value with interpretation at Sungai

    Batu study area.

    70

    Table 4.6 Laboratory test for Bukit Relau study area.

    82

    Table 4.7 Particle size distribution analysis result at Bukit Relau study

    area.

    83

    Table 4.8 Mean and standard deviation of Bukit Relau soil samples.

    83

    Table 4.9 Summary of resistivity value with interpretation and features

    found at Bukit Relau study area.

    86

    Table 4.10 Summary of chargeability value with interpretation and

    features found at Bukit Relau study area.

    87

    Table 4.11 Laboratory test for Air Hitam study area.

    94

    Table 4.12 Summary of resistivity value with interpretation and features

    found at Air Hitam study area.

    94

    Table 4.13 Summary of chargeability value with interpretation and

    features found at Air Hitam study area.

    95

    Table 4.14 Categories of resistivity value obtained in this research.

    101

    Table 4.15 Categories of chargeability value obtained in this research.

    101

    Table 4.16 Summary of result obtained from Sungai Batu study area.

    102

    Table 4.17 Summary of result obtained from Bukit Relau study area.

    103

    Table 4.18 Summary of result obtained from Air Hitam study area.

    103

    Table 4.19 Summary of empirical correlation between geophysical data,

    laboratory tests and rainfall distribution.

    104

  • ix

    Table 5.1 Summary of slope failure potentials and the factor for failure

    at the study areas.

    108

  • x

    LIST OF FIGURES

    Page

    Figure 2.1 ERT profiles through Buzad landslide in (a) 2007 (b) 2012

    (c) 2014 (Popescu et al., 2014).

    10

    Figure 2.2 Resistivity profiles for ERT1 – ERT3 (Giocoli et al., 2015).

    13

    Figure 2.3 3D fence diagram for resistivity section in Aydin (Drahor et

    al., 2006).

    14

    Figure 2.4 Resistivity profiles according to the location (a) top of

    landslide (b) toe of landslide (Hazreek et al., 2017).

    18

    Figure 2.5 a) Average rainfall at Cameron Highland from March 2008

    to Dec 2008 b) Observed total displacement at Prisms I-VI

    (Khan et al., 2010).

    20

    Figure 2.6 Safety factor caused by combination of rainfall and the

    water level fluctuation (Liu and Li, 2015).

    22

    Figure 2.7 The flow of current from a point current source (current

    electrode) and the resulting potential distribution within the

    subsurface (Loke, 2001).

    28

    Figure 2.8 Equilibrium ion distribution (left). Polarization in the

    electric field direction (right) (Slater and Lesmes, 2002).

    29

    Figure 2.9 Principle of time domain IP signal (a) current on – off (b)

    the measured voltage decay (modified from Slater and

    Lesmes, 2002).

    30

    Figure 3.1 Location of study areas (Google Earth, 2018).

    35

    Figure 3.2 General geology of Penang Island (Ong, 1993).

    36

    Figure 3.3 Lineament map of Penang Island (Ong, 1993).

    37

    Figure 3.4 Location of study areas on topography map.

    38

    Figure 3.5 Slope in degree for cell 10 units of Penang Island with

    study area locations (Azmi, 2014).

    39

    Figure 3.6 Rainfall distribution from 2014 to 2016 (Department of

    Meteorological Malaysia, 2018).

    40

    Figure 3.7 Number of days with daily amount of rainfall more or equal

    to 20 mm/day in 2014 – 2016.

    41

  • xi

    Figure 3.8 Aerial view of Sungai Batu survey line (Google Earth,

    2018).

    43

    Figure 3.9 Aerial view of Bukit Relau survey line (Google Earth,

    2018).

    44

    Figure 3.10 Aerial view of Air Hitam survey line (Google Earth, 2018).

    44

    Figure 3.11 Soil laboratory test equipment.

    45

    Figure 3.12

    PSD analysis equipment.

    47

    Figure 3.13

    The position of current electrodes (C1 and C2) and

    potential electrodes (P1 and P2) (Loke, 2001).

    52

    Figure 3.14 Electrode configurations of 2D resistivity method (Loke,

    2001).

    53

    Figure 3.15 Wenner-Schlumberger electrode arrangement. The ‘n’

    factor is the dipole separation factor (Loke, 2001).

    53

    Figure 3.16 2D resistivity and IP methods equipment.

    56

    Figure 3.17 2D resistivity method setup on field.

    57

    Figure 4.1 Rainfall distribution at Sungai Batu. (a) Seven days

    cumulative rainfall (b) Rainfall distribution on 6th day and

    7th day.

    68

    Figure 4.2 Inversion model of (a) 2D resistivity and (b) induced

    polarization method at Sungai Batu study area.

    71

    Figure 4.3 2D resistivity inversion model for August 2016 at Sungai

    Batu.

    72

    Figure 4.4 2D resistivity inversion model for September 2016 at

    Sungai Batu.

    72

    Figure 4.5 2D resistivity inversion model for November 2016 at

    Sungai Batu.

    73

    Figure 4.6 2D resistivity inversion model for December 2016 at

    Sungai Batu.

    74

    Figure 4.7 2D resistivity inversion model for January 2017 at Sungai

    Batu.

    74

    Figure 4.8 Sungai Batu weathered granite zone changes throughout the

    monitoring period.

    76

  • xii

    Figure 4.9 Monitoring resistivity values at distance 30 – 80 m at

    Sungai Batu study area.

    77

    Figure 4.10 Sungai Batu weak zone changes during the monitoring

    period.

    78

    Figure 4.11 Monitoring resistivity values at distance 90 – 120 m at

    Sungai Batu study area.

    79

    Figure 4.12 Sungai Batu granitic bedrock changes throughout the

    monitoring period.

    80

    Figure 4.13 Monitoring resistivity values at distance 110 – 150 m at

    Sungai Batu study area.

    81

    Figure 4.14 Rainfall distribution at Bukit Relau. (a) Seven days

    cumulative rainfall (b) Rainfall distribution on 6th day and

    7th day.

    85

    Figure 4.15 Inversion model of (a) 2D resistivity and (b) induced

    polarization method at Bukit Relau study area.

    88

    Figure 4.16 2D resistivity inversion model for September 2016 at Bukit

    Relau.

    89

    Figure 4.17 2D resistivity inversion model for November 2016 at Bukit

    Relau.

    89

    Figure 4.18 2D resistivity inversion model for December 2016 at Bukit

    Relau.

    90

    Figure 4.19 2D resistivity inversion model for January 2017 at Bukit

    Relau.

    91

    Figure 4.20 Bukit Relau fracture changes throughout the monitoring

    period.

    92

    Figure 4.21 Monitoring resistivity values of distance 50 – 80 m at Bukit

    Relau study area.

    93

    Figure 4.22 Inversion model of (a) 2D resistivity and (b) induced

    polarization method at Air Hitam study area.

    96

    Figure 4.23 Empirical correlation between porosity and moisture

    content at Sg Batu and Bukit Relau study area.

    97

    Figure 4.24 Empirical correlation between resistivity and soil

    laboratory tests.

    98

  • xiii

    Figure 4.25 Empirical correlation between chargeability and soil

    laboratory tests.

    99

    Figure 4.26 Empirical correlation of resistivity and cumulative rainfall

    of seven days including the survey day.

    100

    Figure 4.27 Empirical correlation of chargeability and cumulative

    rainfall of seven days including the survey day.

    100

  • xiv

    LIST OF ABBREVIATIONS

    2D Two dimension

    3D Three dimension

    4D Four dimension

    ALERT Automated time – lapse electrical resistivity

    tomography

    ASTM American Society for Testing and Materials

    BS British Standard

    C1/C2 Current electrode

    ERT Electrical resistivity tomography

    FOS Factor of safety

    GIS Geographic information system

    IP Induced polarization

    NPP North Penang Pluton

    NW Northwest

    P – wave Primary wave

    P1/P2 Potential electrode

    PSD Particle size distribution

    RES2DINV Resistivity two-dimension inversion

  • xv

    RMS Root mean square

    S – wave Secondary wave

    SE Southeast

    SK Sekolah Kebangsaan

    SMK Sekolah Menengah Kebangsaan

    SP Self – potential

    SPP South Penang Pluton

    SW Southwest

    TLERT Time lapse electrical resistivity tomography

    USCS Unified Soil Classification System

  • xvi

    LIST OF SYMBOLS

    Vm measured voltage

    Vr residual voltage

    ρa apparent resistivity

    ∆t length of the time window of integration.

    ∇ gradient operator

    △V Potential difference

    Cc Coefficient of curvature

    Cu Coefficient of uniformity

    d diameter

    D Effective size

    E electric field intensity

    e void ratio

    I current

    k geometric factor

    M chargeability

    ƞ Porosity

    r distance of point in the medium

    R Coefficient of correlation

  • xvii

    R resistance

    R2 Coefficient of determination

    V electric potential

    w Moisture content

    ρ resistivity

    ρbulk Bulk density

    σ conductivity

    ϕ phi unit

  • xviii

    PENILAIAN KEGAGALAN CERUN DI PULAU PINANG MENGGUNAKAN

    KAEDAH GEOELEKTRIK

    ABSTRAK

    Kegagalan cerun di kawasan berbukit dan kawasan cerun tidak berkurang

    setiap tahun. Hal ini boleh membahayakan penduduk setempat. Walau bagaimanapun,

    cerun tidak hanya terhad di kawasan penempatan tetapi juga boleh dilihat di sepanjang

    lebuhraya dan jalan persekutuan. Kajian ini bertujuan untuk menyiasat cerun di

    kawasan berisiko tinggi di Pulau Pinang (Sungai Batu, Bukit Relau dan Air Hitam)

    menggunakan kaedah keberintangan 2D dan polarisasi teraruh serta menganalisa dan

    mengaitkan keputusan dari keadah keberintangan 2D, kaedah polarisasi teraruh, ujian

    makmal dan taburan hujan untuk potensi kegagalan cerun. Kawasan – kawasan kajian

    dipilih berdasarkan kepada kajian terdahulu dan kes – kes kegagalan cerun yang

    dilaporkan berlaku di Pulau Pinang. Berdasarkan kepada keputusan, kebarangkalian

    untuk kegagalan cerun di Sungai Batu adalah disebabkan oleh kewujudan zon lemah

    dengan nilai keberintangan rendah 0 – 400 Ωm and nilai kebolehcasan rendah < 3 ms

    manakala Bukit Relau pula dijangka mengalami kegagalan cerun disebabkan oleh zon

    luluhawa dengan nilai keberintangan pertengahan 750 – 3000 Ωm dan nilai

    kebolehcasan pertengahan 3 – 10 ms. Kewujudan rekahan juga menyumbang kepada

    kegagalan cerun terjadi. Sungai Batu dan Bukit Relau terletak berhampiran dengan

    sesar, sekaligus meningkatkan potensi kegagalan cerun disebabkan oleh ciri – ciri

    batuan yang kekar dan ricih. Air Hitam dikenalpasti terdedah kepada kegagalan cerun

    disebabkan oleh kewujudan zon lempung tepu berdasarkan nilai keberintangan yang

    rendah (< 400 Ωm) tetapi nilai kebolehcasan yang tinggi (> 25 ms). Ujian makmal

    tanah juga dilakukan untuk mengenalpasti kandungan air dan keliangan. Pengamatan

  • xix

    kolerasi antara nilai keberintangan dan nilai kebolehcasan diperoleh dari kaedah

    geofizik dengan kandungan air dan keliangan dari ujian makmal tanah adalah berkadar

    songsang antara satu sama lain dengan kekuatan kolerasi kuat sehingga sangat kuat.

    Analisis taburan saiz zarah berjaya mengenalpasti tanah di Sungai Batu dan Bukit

    Relau adalah pasir berkelikir. Cerun – cerun dipantau selama beberapa bulan untuk

    memerhati sebarang perubahan sub permukaan. Berdasarkan keputusan di Sungai

    Batu, zon lemah dengan nilai keberintangan < 400 Ωm ditemui di tengah garis tinjauan

    manakala zon luluhawa dengan nilai keberintangan 500 – 3000 Ωm dikenalpasti

    sepanjang garis tinjauan. Kaedah keberintangan 2D mendapati nilai yang menurun, ini

    menunjukkan zon – zon yang semakin longgar. Rekahan juga dikesan terbentuk

    semasa tempoh pantauan di jarak 130 – 140 m. Di Bukit Relau, fenomena yang sama

    dapat diperhati dimana nilai keberintangan menurun dengan masa. Rekahan yang

    dikesan di jarak 60 m bertambah lebar berbanding di awal tempoh pantauan dan

    sebuah lagi rekahan dikesan terbentuk di garis tinjauan. Pemantauan cerun

    membuktikan sub permukaan mengalami perubahan dan ia dipengaruhi oleh pelbagai

    faktor seperti hujan di sepanjang bulan. Kajian ini berjaya mengenalpasti potensi

    kegagalan cerun di kawasan – kawasan kajian iaitu zon lemah dan kehadiran bahan

    lempung di Sungai Batu, zon luluhawa granit di Bukit Relau dan zon lempung tepu di

    Air Hitam. Faktor yang membawa kepada kebarangkalian kegagalan cerun di kawasan

    – kawasan kajian ialah keadaan tanah yang telap, taburan hujan yang tinggi dan juga

    kesan luluhawa.

  • xx

    SLOPE FAILURE ASSESSMENT IN PENANG ISLAND USING

    GEOELECTRICAL METHODS

    ABSTRACT

    Slope failures never cease to end in hilly and slope area every year. This is very

    dangerous especially for those who lives within the proximity. However, slope is not

    only found in residential area but also alongside highways and federal roads. This

    research aims to investigate slope at the selected highly suspected area in Penang

    Island (Sungai Batu, Bukit Relau and Air Hitam) using 2D resistivity and induced

    polarization methods and to analyse and correlate the results from 2D resistivity

    method, induced polarization method, laboratory tests and rainfall distribution for

    slope failure potentials. The study areas were selected based on the previous studies

    and cases of slope failure reported in Penang Island. Based on the results, Sungai Batu

    has probability for slope failure due to weak zone with low resistivity value of 0 – 400

    Ωm and low chargeability of < 3 ms while Bukit Relau was expected to have slope

    failure due to the weathering zone with intermediate resistivity 750 – 3000 Ωm and

    intermediate chargeability 3 – 10 ms. The existence of fractures also contributed to

    trigger the slope failures. Sungai Batu and Bukit Relau are located near faults and thus,

    intensified the slope failure potential due to highly jointed and sheared rocks

    characteristic. Air Hitam was determined to be vulnerable to slope failure due to the

    presence of clay saturated zone indicated by low resistivity value (< 400 Ωm) but high

    chargeability value (>25 ms). Soil laboratory tests were also conducted to determine

    the moisture content and porosity. The empirical correlation of resistivity and

    chargeability values obtained from geophysical methods with moisture content and

    porosity from soil laboratory tests indicated that they are inversely proportional to each

  • xxi

    other with strength of correlation range from strong to very strong. PSD analysis

    successfully determined that the soil at Sungai Batu and Bukit Relau are gravelly sand.

    The slopes were also monitored for several months to observe any changes within the

    subsurface. Based on the results at Sungai Batu, weak zone with resistivity of < 400

    Ωm was found at the centre of survey line while weathered zone with resistivity 500 –

    3000 Ωm was identified along the survey line. 2D resistivity method recorded

    decreases in value therefore indicated that the zones were becoming loose. A fracture

    was also detected formed during the monitoring period at distance 130 – 140 m. As

    for Bukit Relau, the same phenomenon was observed where the resistivity value

    decreased with time. Fracture found at distance 60 m is wider since the beginning of

    monitoring period and another fracture was observed to develop at distance 140 m

    along the survey line. Monitoring the slope proved that the subsurface experience

    changes and can be affected by various factors such as rainfall over the months. This

    research has successfully determined slope failure potentials in the study areas which

    are the weak zone and presence of clayey material at Sungai Batu, weathered granite

    zone at Bukit Relau and clay saturated zone at Air Hitam. Factors that leads to slope

    failures possibilities in the study areas are the permeable soil condition, high rainfall

    distribution and also weathering effect.

  • 1

    CHAPTER 1

    INTRODUCTION

    1.0 Preface

    Reported from cases of landslides, rockfalls and other types of slope failures

    never cease to end every year. In the worst case, some of the slope failure repair

    methods such as retaining walls, rock bolts and geo grid had collapsed together with

    the slope failures. This perpetual issue will require an amount of money to be taken

    care of.

    Slope is not an uncommon structure in Malaysia. It can be seen alongside the

    highways, federal roads and also residential areas. About 5000 km of the trunk roads

    in Malaysia involved many cut slopes and traversed on hilly and mountainous area.

    Approximately about 75% of the roads are underlain by granitic formation while the

    other 25% of the roads are underlain by meta – sediments formation such as the

    mudstone, sandstone and siltstone. Numbers of slope failure occurrences happen on

    the mountainous roads especially during the rainy season which leads to traffic

    disruption, injuries and also loss of lives (Singh et al., 2008). Although it happens

    frequently, an absolute prevention method has yet to be found. Table 1.1 shows the

    major slope failure occurrences in Malaysia in from 2002 – 2017.

    Table 1.1: Series of major slope failure occurrences in Malaysia and consequences in

    terms of deaths from 2002 – 2017.

    Date Location Coordinate

    Deaths Sources Longitude Latitude

    20 November

    2002 Taman Hillview, Hulu Klang 101.761500 3.175442 8

  • 2

    Continuation of Table 1.1

    29 November

    2004 KM 59, Kuala Lipis – Merapoh 101.961883 4.487183 4

    Dep

    artm

    ent

    of

    Pu

    bli

    c W

    ork

    s M

    alay

    sia

    2 December

    2004 Taman Bercham Utama, Ipoh 101.135061 4.645389 2

    31 May 2006 Kg Pasir, Hulu Klang, Selangor 101.764778 3.206783 4

    26 June 2006 KM 8.5, Pelabuhan Sepanggar,

    Kota Kinabalu, Sabah 116.674689 6.095556 1

    30 November

    2008

    Ulu Yam Perdana, Kuala

    Selangor 101.674689 3.389919 2

    6 December

    2008

    Taman Bukit Mewah, Bukit

    Antarabangsa, Hulu Klang 101.769722 3.186111 5

    16 January

    2009 Bukit Kanada, Miri, Sarawak 113.996494 4.393056 2

    29 January

    2011 Sandakan, Sabah 118.127078 5.847014 2

    21 May 2011 Rumah Anak Yatim At –

    Taqwa, Hulu Langat 101.814444 3.138611 16

    7 August 2011 Perkampungan Orang Asli Sg

    Ruil 101.370464 4.487361 7

    p18 February

    2012 Kg Terusan, Lahad Datu, Sabah 118.359314 5.048847 2

    3 July 2013 Ukay Perdana, Selangor - - 3

    Kazmi

    et al.

    (2016)

    16 July 2013 Kampung Mesilau, Kundasang - - 1 Utusan

    30 December

    2014 KM Jalan Brinchang – Tringkap - - 2

    Astro

    Awani 31 December

    2014

    Kampung Raja, Cameroon

    Highland - - 1

    22 October

    2017 Tanjung Bungah, Penang - - 14 Reuters

    Shallow slide is the most common type of slope failure in Malaysia where the

    slide surface is usually less than 4 m depth and occurs during or immediately after

    intense rainfall (Jawaid, 2000). Other types of slope failure found are deep-seated

    slide, debris flow and geologically controlled failures such as wedge failures and rock

    falls.

    By definition from Frasheri (2012) slope is a dynamic system of geo-

    environment phenomena that are related to the movement of soil and rock masses.

    Some examples of slope failure including avalanche of the rocks, debris and soil flow,

    collapse of the blocks and landslides. Slope failure phenomena can be defined as an

  • 3

    engineering and environmental issue. In order for a slope to fail, there is a process

    related to deformation of the rock mass, accumulation of stress and mineralogical

    changes involved. The body movement only occurs as the last stage and associated

    directly with mechanical and geological condition of the rock mass. The slope become

    unstable as the rock mass loss mechanical stability due to full compliance of the

    unstable condition. The rock mass sensitivity to the external force also increased as it

    become more unstable.

    There are many factors that affected slope stability therefore causes slope

    failure to occur. One of the factor is due to gravitational force which pulls everything

    to the direction of Earth’s centre. Unstable rock or structure will allow the gravitational

    force to act and end up as landslide or rockfall. Another major factor that influences

    slope stability is water. Additional of water on the subsurface will results as the slope

    to increase in weight therefore becomes unstable. Oversaturated soil with water will

    cause the grain to lose contact to one another and can also change the angle of repose.

    The nature of Earth material such as clayey type of soil and the presence of structure

    such as fracture and weathered zone in the subsurface can also cause slope failure to

    occur. On top of all, the most critical factor for slope failure to occur is triggering

    events such as heavy rainfall and earthquake (Nelson, 2013).

    1.1 Problem statements

    Aside from the slope at the roadsides, residential areas and agricultures are

    developed on the slope areas too. The limited flat land in Penang Island has urged

    developers to develop buildings on the steep slopes (Teh, 2000). This irreversible

    action has taken tolls on the hills ecosystems. As the developed slope areas spreads,

    the effects could be more severe and worse. On top of that, illegal forest clearing and

  • 4

    illegal farming on slopes without any consideration of the subsurface condition could

    accelerate soil erosion and slope failures. Table 1.2 shows the summary of slope

    failures in Penang Island in 2008 to 2017. This indicates that slope failure in Penang

    Island is a crucial matter.

    Table 1.2: Summary of slope failures in Penang Island.

    Date Location Remarks

    4 October 2008 Persiaran Kelicap, Sungai Ara

    Collapsed retaining wall

    caused flooding and

    mudslide to resident houses.

    7 October 2008 Jalan Teluk Kumbar – Balik Pulau Landslide caused road

    closure to traffic

    6 April 2009 Pangsapuri Farlim Tower, Bandar

    Baru Farlim, Air Hitam

    Landslide, damage on

    vehicles

    10 June 2010 Pangsapuri Bandar Baru Air Hitam Landslide

    24 June 2010 Batu Feringghi

    Mudflow and mudslide from

    nearby hillslope

    development project

    10 March 2011 Taman Terubong Jaya

    Landslide, caused collapsed

    of retaining wall and buried

    two cars

    September 2013 Penang Hills Landslide at KM 2.1, KM

    2.5 and KM 4.0

    29 October 2016 Air Hitam

    Landslide near Kek Lok Si

    Temple heading to Air

    Hitam Dam

    7 November 2016 Jalan Ujung Baru, Teluk Bahang Landslide forced road

    closure to traffic

    5 November 2017 Tanjung Bungah Three newly built luxury

    houses destroyed.

    In accordance to slope failure occurrence, Department of Public Work

    Malaysia will act according to Malaysia Standard Code Practice MS 2038: 2006: Site

    Investigation – Code of Practice which included the application of boring log, ground

    water observation and Mackintosh probe test and Malaysia Standard Code Practice

    MS 1056: 2005: Soil for Civil Engineering Purpose – Test Method which included

    laboratory test of disturbed and undisturbed soil samples. Slope failure is a perpetual

    issue in Malaysia, any method that can be in assistance to solve such issue should come

    to the front. In this research, the ability of geophysical methods in dealing with

    engineering and environmental issue are tested to determine the slope failure potential.

  • 5

    The common geophysical methods apply for slope failure studies are 2D

    resistivity method and seismic refraction method (Popescu et al., 2014; Giocoli et al.,

    2015; Muztaza et al., 2017; Hazreek et al., 2017). In this research, the application of

    2D resistivity method is paired with induced polarization method as this combination

    in slope failure studies is yet to be well-known (Marescot et al., 2008).

    1.2 Research objectives

    The objectives of conducting this research is listed as follows:

    i. To investigate slope at the selected highly suspected area in Penang

    Island (Sungai Batu, Bukit Relau and Air Hitam) using 2D resistivity

    and induced polarization methods.

    ii. To analyse and correlate the results from 2D resistivity method,

    induced polarization method, laboratory tests and rainfall distribution

    for slope failure potentials.

    1.3 Scope of research

    This research was conducted at Penang Island which is generally made up of

    granitic rock. The three study areas were chosen based on the landslide distribution in

    Penang Island obtained from previous studies and also cases of landslide reported.

    The geophysical methods used in this study were 2D resistivity method and

    induced polarization (IP) method by using ABEM SAS4000 Terrameter and ABEM

    ES 10-64C electrode selector. The resistivity inversion models were produced by using

    RES2DINV software by Geotomo. Each model inversion was studied and observed so

    that any slope failure possibilities can be detected.

  • 6

    Aside from geophysical methods, the soil laboratory tests were also conducted

    in order to measure the soil porosity, moisture content and particle size distribution.

    Rainfall distribution were also factored, in order to identify the potential of the slope

    failures.

    1.4 Significance of study

    People tend to use the ground methods, geotechnical methods and remote

    sensing over the geophysical methods (Talib, 2003; Ahmad et al., 2006; Khan et al.,

    2010; Lateh et al., 2011; Department of Public Works Malaysia, 2018). There are

    many reasons that geophysical method should be chosen when dealing with

    engineering and environmental issues. The geophysical methods are non – destructive,

    low cost consumption and have wider area coverage. Geophysical methods also have

    the potential in dealing with engineering and environmental problem such as slope

    failures.

    This research aims to apply geophysical methods in dealing with engineering

    and environmental problems Thus, this research is carried out in order to convince the

    potential lies within geophysical methods in dealing with engineering and

    environmental problems.

    By applying geophysical methods in slope study, the expenditure can be

    reduced and remedial works will be done in more efficient ways and not blindfolded.

    The significant of this study is to understand the mechanism of slope failures at highly

    potential areas in Penang Island as most of the study conducted before were site

    specific. Another significant of this study is the application of induced polarization

    method which rarely used for slope study. This aims to detect saturated zone and high

    moisture area in the subsurface and its origin.

  • 7

    1.5 Thesis outlines

    This thesis contained five chapters as follows:

    Chapter 1 is the introduction of the research where the preface of study,

    problem statements, research objectives, scope of study, significance of study, and

    thesis outline are explained.

    Chapter 2 is the literature review. The background of the slope is elaborated,

    theory of 2D resistivity and IP method is explained and the previous study that related

    to this research are discussed.

    Chapter 3 is the materials and methods chapter. The details about the study

    area including the geological of the area and the survey lines orientation are shown.

    This chapter also explained the equipment used and the procedures during data

    acquisition. Aside from that, procedure that related to soil laboratory tests are

    explained as it is part of the research element.

    The results are discussed in Chapter 4. This includes the soil laboratory tests,

    particle size distribution results and geophysical results. The results are correlated to

    the rainfall distribution. Empirical correlation between laboratory test and geophysical

    results are also shown in this chapter.

    Chapter 5 is the conclusion and recommendations. The research findings are

    concluded and discussed. Some recommendations for future works are also suggested

    in this chapter.

  • 8

    CHAPTER 2

    LITERATURE REVIEW

    2.0 Introduction

    For engineering and environmental purposes, people tend to choose the

    airborne and satellite methods such as remote sensing and Geographic Information

    System (GIS) or the direct ground-based techniques such as piezometer and laboratory

    tests over geophysical method which are also capable in solving the engineering and

    environmental problems (Talib, 2003; Ahmad et al., 2006; Khan et al, 2010; Lateh et.

    al, 2011). Fortunately, people had grown interest in geophysical method in order to

    investigate engineering and environmental problems such as slope stability in the last

    several decades (Jongmans and Garambois, 2007; Chambers et al., 2011). Each

    geophysical method has their own specialities on specific targets and environments

    which will produce good results besides time and cost effective. Several studies on

    slope failures and the application of geophysical methods on slope stability are

    included in this chapter.

    2.1 Previous studies

    A landslide on argillaceous material occurred in Western Cameroon around

    Kekem area. Geophysical and geotechnical surveys were carried out by Epada et al.

    (2012) with purpose to understand the triggering processes and mechanism of the

    landslide and to assess the slope stability. Resistivity survey had been conducted by

    using electrode configuration of Schlumberger array in order to monitor the behaviour

    of the landslide in term of resistivity. A zone of low resistivity value was identified as

    clayey sand-filled aquifer in the subsurface of the landslide. This aquifer was suspected

  • 9

    to be the triggering factor of the landslide. Based on the geotechnical sounding result,

    the aquifer had a thickness of 7.0 m whereas the depth of the landslide crest level to

    the failure surface reached 3.0 m and 20.6 m. Next, laboratory tests were carried out

    to evaluate the cohesion of the soil and the angle of internal friction. The tests result

    shows that the soil has low consistency which is almost doughy. As for stability

    analysis, the mean value of the factor of safety (FOS) is 1.4 which was lower that the

    slope stability coefficient which is 1.5. Therefore, the slope was unstable and likely to

    reactivate at any moment.

    A landslide was studied at Buzad village, Timis County, Romania by using

    electrical resistivity tomography (ERT). The landslide occurred in 2006 was

    reactivation of an old landslide. Popescu et al. (2014) conducted three resistivity

    survey over the main body of the landslide by using electrode configuration of Wenner

    array in 2007, 2012 and 2014 (Figure 2.1). The length of the profile was 90 m in 2014

    but 100 m in 2007 and 2012 and achieved depth of about 15.0 m along all longitudinal

    profiles. The results showed that a section with resistivity value of 0-35 Ωm at the

    upper half while the middle part ranged from 55 – 100 Ωm. The bottom part recorded

    as shallow high resistivity zone. This suggest that high water content from the middle

    part of the profile may be the triggering factor of the reactivation. The hypothesis was

    confirmed from an in-situ observation of the ground water table appeared to the

    surface. Whereas the high resistivity value of the bottom part is compact material

    (sands) embedded in clayey matrix of the old landslide body. Resistivity method

    allows one to identify high water content area that cause the reactivation and thus

    reconstruction of the landslide body including the body materials in movement and its

    volume. Aspect noted in all resistivity profiles, the new and old landslide were located

    in a zone of obviously changing resistivity values.

  • 10

    Figure 2.1: ERT profiles through Buzad landslide in (a) 2007 (b) 2012 (c) 2014

    (Popescu et al., 2014).

    Glacial erosion had produced ‘crag and tail’ structure at the Edinburgh Castle

    which is one of the most important heritage site in Scotland. The crag consists of

    columnar jointed basal that formed a gentle slope protecting the tail of sediment from

    glacial erosion. An apparent instability was observed in the southern side of the ‘tail’

    between the Edinburgh Castle Esplanade and Johnston Terrace in 1997 which later

    initiated the geotechnical and geological investigation on the particular slope including

    (a)

    (b)

    (c)

  • 11

    electrical resistivity survey. In order to determine the subsurface structures and

    variations in pore fluid distribution within the slope, Donnelly et al. (2005) conducted

    six resistivity survey lines with length of 24 m with electrode configuration of Wenner

    array. Line 1 to Line 5 were positioned down the slope perpendicular with the southern

    boundary wall of Esplanade whereas Line 6 was positioned across the slope parallel

    to the Esplanade wall. A shallow slope failure was confirmed based on the result

    however the initial date of failure is not known but likely since at least 1950’s. The

    resistivity profiles indicated that the instability was due to zones of low resistivity and

    high saturation. The backscarp also seems to be associated with relatively thin clay

    layer which apparently not a slip plane but however may cause the local groundwater

    to flow in as a highly permeable fill material. Similar condition was found to the east

    and west of the uppermost featured of the landslide lateral continuation.

    Giocoli et al. (2015) performed a joint analysis of geophysical surveys, aerial

    photos interpretation, morphotectonic investigation, geological field survey and

    borehole data to investigate an area in the Montemurro territory in southeastern sector

    of High Agri Valley (Basilicata Region, southern Italy). Generally, the area consists

    of steep slopes, encased streams within narrow and deep land incision and abrupt

    acclivity change due to tectonic structures or lithological variation. This area has been

    affected by the hydrogeological instability which included active and inactive

    landslides. Surficial investigation identified the existing of northwest (NW) –

    southeast (SE) trending and southwest (SW) facing scraps between villages of Pergola

    to the north and Voggioni to the south. Geophysical surveys were conducted to unravel

    the surface expression of the strand. Three resistivity survey lines were carried out

    across the NW-SE scarp by using Wenner-Schlumberger electrode configuration with

    20 m spacing. Survey line ERT1 and ERT3 achieved depth of penetration of 150 m

  • 12

    with spread of 940 m length whereas survey line ERT2 achieved the same depth with

    spread of 1100 m length (Figure 2.2). In the upper of line ERT2, a body associated

    with the Verdesca landslide was identified between 430 m and 1100 m based on the

    resistivity values (25 – 70 Ωm). The estimated thickness was derived from borehole

    data GB1 – GB3 and resistivity contrast from ERT2, varies from less than 10 m and

    up to 30 m. Another geophysical method done was a high-resolution seismometer with

    24-bit dynamic was aimed at the very low amplitude range. Thirty-five ambient noise

    measurements with each duration of 12-15 minutes with additional measurements

    overlap with all resistivity profile lines were taken. The results successfully showed

    the fundamental frequency was related to the depth variation of the seismic impedance

    differ between the low resistive Quartenary continental deposits (QD) and Albidona

    Formation (AF) and high resistive Gorgoglione Flysch (GF). These joint analyses

    succeed in achieving the objectives of the study which is to image the shallow

    geological and structural setting as well as to verify the nature of the NW-SE scarps

    and thus interpreting it as surface expression of the Montemurro Fault.

  • 13

    Figure 2.2: Resistivity profiles for ERT1 – ERT3 (Giocoli et al., 2015).

    A study of landslide was conducted by Drahor et al. (2006) at district of Aydin,

    Turkey in 2003 on a slope next to a newly built school building. The slope was unstable

    due to an excavation work and heavy rainfall. Three resistivity survey lines were

    conducted over the landslide using Wenner electrode array resulting on the geometry

    and characteristic of the landslide. Eight boreholes were also carried out on the

    landslide. Both methods showed a fault presence at the area with addition of a surface

    rupture indicated by the resistivity profiles (Figure 2.3).

  • 14

    Figure 2.3: 3D fence diagram for resistivity section in Aydin (Drahor et al., 2006).

    Resistivity and self-potential methods were applied to study the hydraulics of

    landslide process as these methods are capable to provide spatial and volumetric

    information as well as sensitive toward hydraulic changes in the subsurface. A system

    called Automated Time-lapse Electrical Resistivity Tomography (ALERT) was

    applied on an active landslide near Malton, North Yorkshire, United Kingdom in order

    to develop a 4D landslide monitoring system that capable to characterise the

    subsurface structure of landslide and detecting the hydraulic precursor to movement.

    According to Chambers et al. (2009), the time-lapse resistivity imaging was able to

    show the changes related to the seasonal temperature variation, moisture content and

    ground movement within the landslide. The 4D resistivity imaging was an effective

    method to investigate the hydraulic of a landslide whilst taking the influence of

    temperature and electrode displacement into consideration.

    One of study conducted in Malaysia is to investigate the influence of natural

    slope geomorphology on active cut slope failure near Gunung Pass, Simpang Pulai-

    Lojing Highway by Shuib et al. (2012). Previous studies have found out that there was

    close correlation between the relict landslide scars on the natural slope and the

  • 15

    presence of cut slope instabilities. Hence resistivity and seismic refraction surveys

    were conducted across the relict landslide scars. Based on the results, the steep relict

    scarps were connected at the subsurface by a circular slip surfaces which is represent

    by steep weak zones. The head scarp zone was represented by the topmost slip surfaces

    with tension cracks suggestive of extensional strains while the toe region was

    represented by the reversed slip surface suggestive of compressional strains. The

    failure was due to the head and the upper main body zone sliding roughly orthogonal

    to the foliation while the middle and toe zone is sliding down and out of the foliation.

    From the surface and subsurface observation, the natural slope was inferred to be

    creeping which later induces shallow planar and circular failures at the cut slope.

    Based on a study conducted by Chigira et al. (2011), landslides in weathered

    granitic rocks are greatly influence by the type of weathering and it is site specific. The

    mechanism of failure in deep weathering profiles in Malaysia are highly controlled by

    the nature of the weathered material and its mass structure. In Japan, the landslides

    occurred due to moderately weathered decomposed granite. The rock loosened rapidly

    as it was exposed to the ground surface and formed loosened layers to slide. The fact

    of weathered granite is prone to slide was known for many years. However, the

    landslide mechanism was not yet fully understood due to the weathering profile was

    site specific and differ among climates. More than 80 landslides occurred along the

    mountainous main highway to Genting Sempah, Pahang. Most of the landslides

    occurred in a few hours in June 1995 as there was a continuous rain for more than 72

    hours. Majority of the landslide can be categorized as small to medium size with

    sliding materials less than 500 m3. Types of slope failure included shallow and deep

    sliding, rock block sliding and debris flow. This is a region that formed by granite

    batholiths and the granite has undergone intensive tropical weathering. This resulting

  • 16

    in forming weathered profiles with various characteristic and thickness. Most of the

    landslides are related to the weathered materials. The intense and heavy rain saturate

    the residual soil thus, triggering two major landslides upstream of a tributary of Sungai

    Gombak.

    A study conducted by Komoo (1997) at Bukit Antarabangsa concluded that

    the weathered granitic material may contributed to landslide as it was porous, easily

    crumble and inherited the plane of weakness from the parent rock. Bukit Antarabangsa

    has marked in the history of Malaysia landslide disasters as there were six major

    landslides occurred since 1993. The hill was underlain by granite and extensive

    weathering has transformed the granite into residual soil (grade VI) and completely

    weathered material (grade V). The weathered material was sandy with average

    thickness profile of 30 m. The subsurface loose its consistency with increasing amount

    of water. This condition triggered a collapsed of twelve storey Highland Tower

    condominium in 1993.

    Another study conducted by Komoo and Lim (2003) at the same Bukit

    Antarabangsa with 100 m distance south from the previous landslide. In 2002, a

    bungalow was destroyed due to landslide killing eight people. The landslide

    mechanism was rather complex but it is due to continuous heavy rain that triggered

    the sliding. That was not all, other factors may also contribute the triggering of the

    landslide. Factors such as weathered granitic materials that prone to failure, geological

    lineament that facilitating the sliding. An old landslide landform found nearby also

    aided the accumulation of groundwater that resulting in the landslide in 2002.

    Muztaza et al. (2017) has conducted a slope failure evaluation and landslide

    investigation by using 2D resistivity method in Selangor. Nine survey lines were

  • 17

    carried out at Site A and another six survey lines at Site B with minimum electrode

    spacing of 5 m were performed using Pole – Dipole electrode array. Alluvium or

    highly weathered zone with resistivity value of 100 – 1000 Ωm found at depth > 30 m,

    saturated area with resistivity value of 1 – 100 Ωm and boulders with resistivity value

    of 1200 – 7000 Ωm. The granitic bedrock was identified with resistivity value of >

    7000 Ωm (Table 2.1). From this study, the triggering factors for slope failure was due

    to the saturated zones, highly weathered zone, highly contain of sand, and boulders.

    Table 2.1: Summary of resistivity value with interpretation at the study areas in

    Selangor (Muztaza et al., 2017).

    Resistivity value (Ωm) Interpretation

    1 – 100 Saturated zone

    100 – 1000 Alluvium or highly weathered zone

    1200 – 7000 Boulder

    > 7000 Granitic bedrock

    A slope failure in Kenyir Lake was evaluated by Hazreek et al. (2017) using

    resistivity method with a reference to a borehole data. Two resistivity survey line was

    carried out using electrode array of Schlumberger array. The main factor that triggered

    the slope failure is the combination of heavy rainfall and the presence weakness zone.

    The results also successfully detected fault and rock discontinuities which associated

    by low resistivity value (Figure 2.4). By applying resistivity method, the shape and

    depth of subsurface landslide that caused ground damage can be determined easier as

    the resistivity method mapped the subsurface profile based on the resistivity values.

  • 18

    Figure 2.4: Resistivity profiles according to the location (a) top of landslide (b) toe of

    landslide (Hazreek et al., 2017).

    Yaccup and Tawnie (2015) had conducted a comparison between resistivity

    imaging technique and borehole data on determining depth of granite body as the

    active quarry site in order to define the accuracy of the resistivity data with borehole

    information. Eight resistivity profiles were built near to several boreholes with

    maximum distances of less than 50 m. The result shows that in the tropical region such

    as Malaysia (Table 2.2), the resistivity value of low weathered granite to fresh granite

    is more than 5000 Ωm, medium weathered between 1000 – 5000 Ωm and highly

    weathered granite is lower than 1000 Ωm. Resistivity and borehole recorded accuracy

    more than 80% with another 20% error due to changing of resistivity due to existence

    of water, fractured zone and the distance between the survey line and borehole.

    Table 2.2: Resistivity range of weathered granite and fresh granite in Malaysia

    (Yaccup and Tawnie, 2015).

    Resistivity value (Ωm) Interpretation

    < 1000 Highly weathered granite

    1000 – 5000 Medium weathered granite

    > 5000 Low weathered – fresh granite

    (a)

    (b)

  • 19

    Jinmin et al, (2013) applied 2D resistivity method for subsurface study at

    Bukit Bunuh. The aim was to identify the bedrock structure, fracture of shallow

    subsurface and identify the alluvium pattern. Due to large study area, the borehole data

    is not adequate to measure the subsurface condition. Therefore, the borehole data were

    used as preliminary information to refine 2D resistivity results. A survey line of 2.065

    km was done by applying Pole – Dipole array with 5 m minimum electrode spacing.

    The results show two major zones in the study area; resistivity value of 10 – 800 Ωm

    interpreted as alluvium and resistivity value of more than 3000 Ωm as boulder and

    granitic bedrock.

    A study on hill-slope movement was conducted by Khan et al. (2010) to

    monitor a land movement during rainy seasons in 2008. Two landslides occurred

    between 23 and 26 km stretched through Gunung Pass, Cameron Highland in April

    and December 2007 respectively. Based on deduction, the hilly terrain was triggered

    by the rainfall events. Moreover, the slope at Gunung Pass may experience some

    movement within the subsurface from the past rainfall events before the failure

    occurred in 2007. Therefore, a theodolite study was conducted on the slow hill-slope

    movement to monitor the land movement during rainy seasons of 2008. The results

    successfully identified a close correlation between the hill-slope displacements and the

    rainfall amount during the study period. The slow hill-slope movement occurred after

    a heavy rainfall in 2008. Result from Prism III theodolite showed that the down slope

    movement was more than 4 m, southward movement of 1.94 m and westward

  • 20

    movement of more than 5 m (Figure 2.5). As conclusion, the area was unstable and

    prone to slide.

    Figure 2.5: a) Average rainfall at Cameron Highland from March 2008 to Dec 2008 b)

    Observed total displacement at Prisms I-VI (Khan et al., 2010).

    Xu et al. (2016) investigate a landslide in southwestern China by using time –

    lapse electrical resistivity tomography (TLERT) in November 2013 and August 2014.

    The study aims to investigate the subsurface hydrogeological environmental and

    evolution of landslides based on the electrical structure and geometry of sliding

    surface. The landslide mechanism is inferred based on the spatiotemporal

    characteristic of the surface water infiltration and groundwater flow within the

    (a)

    (b)

  • 21

    landslide body. The resistivity inversions accurately defined the interface between the

    Quarternary sediments and bedrock when combined with borehole data. The results

    show that the surface water penetrates via the fracture zone and fissures into the

    slipping body and drained as fissure water in the fractured bedrock. This eventually

    caused the weathered layer to soften and erode. This finding indicated that the TLERT

    monitoring able to provide preliminary information on critical sliding and can be used

    for landslide stability analysis and prediction.

    A study conducted by Rahardjo et al. (2001) in Nanyang Technology

    University Campus successfully indicated that the landslides were initiated by the

    rainfall infiltration. The daily rainfall and the cumulative rainfall both act as the

    triggering factor for slope failure. A five days cumulative rainfall with more than 60

    mm combined with daily rainfall exceeded than 90 mm was sufficed to initiated a

    landslide.

    A water – seepage coupling model and stability analysis was developed to

    study the effect water on the soil – slope stability by Liu and Li (2015). In order to

    analyse the effect of water seepage which came from rainwater and water level

    fluctuation, safety factor of slope by rainfall and water level fluctuation was simulated.

    The simulated result indication that both rainfall and water level fluctuation decreased

    slope stability according to the safety factor of the slope (Figure 2.6). The reason for

    this phenomenon is increased in total soil weight and slight improvement of pore

    pressure in slip surface. Therefore, slope stability is highly affected by rainfall and

    water level fluctuation.

  • 22

    Figure 2.6: Safety factor caused by reservoir water, rainfall and combination of rainfall

    and reservoir water fluctuation (Liu and Li, 2015).

    Lateh et al. (2011) monitored the slope movement before the slope failure

    occurs by using inclinometer, piezometer and rain gauge at 3.9 km Jalan Tun Sardon,

    Penang. The soil was detected move on 30th July 2010 and 4th November 2010 due to

    the intense rainfall before the occurrence. Therefore, the soil movement and rainfall

    intensity can be related in affecting slope failure occurrence.

    A slope investigation was carried out at Fraser’s Hill due to a debris flow was

    found at 9 km of Fraser Hill road by Ghazali et al. (2013). Using resistivity method,

    three survey lines parallel to the slope and two survey lines perpendicular to the slope

    were applied at the reported area. Results showed existence of granite body at the

    central part of the east line and nearest to the ground surface. The presence of

    resistivity less than 600 Ωm within the granite body is interpreted as highly fractured

    and water conducting zones. The same zone was detected at east – west and north

    south lines. Therefore, the fracture granite is virtually floating above the water

    saturated zone thus, considered as unstable.

    F

    ac

    tor

    of

    sa

    fety

  • 23

    Ng et al. (2015) has utilized resistivity method to investigate a slope failure at

    Precinct 9, Putrajaya with aided by borehole sampling data. Results showed two zones

    were encountered, high water content zone with resistivity value of 10 – 300 Ωm and

    dry zone with resistivity value of 300 – 100 kΩm. Borehole sampling recorded

    subsurface condition was range from fresh to highly weathered granite. Rock quality

    designation (RQD) indicated value of 0 – 100 % which show the presence of rock

    fracture that cause seepage flow within the subsurface. Therefore, low resistivity zone

    face risk for slope failure which demand remedial measures.

    Ramadhan et al. (2015) has conducted resistivity method by using electrode

    configuration of Wenner – Schlumberger at Bendanduwur Gajahmungkur Semarang

    to identify landslide slip surface. The results of resistivity method reached to depth of

    14 m and it shows that the lithology of the location consist of soil, clay, sandstone and

    breccia. The contact between clay and sandstone found at depth 1.25 to 6.76 m found

    in the survey lines is interpreted as the slip surface of landslide due to the contact

    indicated disconnection between the layers also known as weak zone. Landslide can

    be expected in this location due to the presence of clay, which is impermeable for water

    to pass through.

    A study by Ahmad et al. (2006) at Paya Terubong on a landslide that occurred

    in 1998. The average thickness of highly to completely weathered granitic soil is found

    to be approximately 30 m. The sampled residual soil consists of gravel (14%), sand

    (55%), silt (18%) and clay (13%) which can also represent as course-grained residual

    soil which is also known to be susceptible to landslide.

    Hashim et al. (2015) used shear box test in order to identify slope failure in

    Penang Island. This study aims to determine the soil shear strength under saturated

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    shear box test for samples taken from slope failure locations. The locations were

    selected from slope failure tragedy sites along Teluk Bahang – Balik Pulau road. The

    summary of shear box test and particle size distribution test (BS 5930: 1990) is as in

    Table 2.3 and Table 2.4 respectively. The results indicated that the slope failures were

    found mostly in gravelly silt soil and the range of cohesion recorded was largest

    compare to others soil.

    Table 2.3: Saturated peak shear box and particle size distribution tests, BS 5930: 1990

    (Hashim et al., 2015).

    Soil types Range of cohesion Range of angle of shearing resistance

    Silt 0.1 – 33.4 22.9 – 47.1

    Very silty sand 0.6 – 8.3 30.7 – 62.4

    Sandy silt 0.0 – 27 18.6 – 52.9

    Very silty gravel 0..8 – 37.5 24.5 – 57.2

    Gravelly silt 0.0 – 40.8 18.1 – 65.8

    Table 2.4: Result of soil classification and particle size distribution test, BS 5930: 1990

    (Hashim et al., 2015).

    Soil

    sample Slope condition

    Percentage (%) Soil classification

    Gravel Sand Silt Clay

    A Unfailed 64.88 18.08 17.04 0.00 Very silty gravel

    B Failure mass 37.92 20.67 41.25 0.16 Gravelly silt

    C Failure scar 36.26 30.16 33.53 0.05 Gravelly silt

    D Failure mass 36.88 24.21 38.67 0.24 Gravelly silt

    E Failure mass 26.19 36.88 36.85 0.08 Gravelly silt

    F unfailed 76.93 7.45 15.50 0.12 Very silty gravel

    A study conducted by Bery (2016) to identify the empirical correlation of soil

    properties of shear strength, moisture content, void ratio, porosity, saturation degree

    and Atterberg’s limit with electrical resistivity values from resistivity tomography

    models. Eleven undisturbed clayey sand soil samples were collected at different

    distances, depths and both infield and laboratory condition. Based on the results, the

    electrical resistivity values were highly influence by the soil properties. A good

    estimation of soil mechanics properties can be obtained from the results of electrical

    resistivity tomography model.